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Lecture Outline Chapter 9 Physics, 4th Edition James S. Walker Copyright © 2010 Pearson Education, Inc. Chapter 9 Linear Momentum and Collisions Copyright © 2010 Pearson Education, Inc. Units of Chapter 9 • Linear Momentum • Momentum and Newton’s Second Law • Impulse • Conservation of Linear Momentum • Inelastic Collisions • Elastic Collisions Copyright © 2010 Pearson Education, Inc. Units of Chapter 9 • Center of Mass • Systems with Changing Mass: Rocket Propulsion Copyright © 2010 Pearson Education, Inc. 9-1 Linear Momentum Momentum is a vector; its direction is the same as the direction of the velocity. Copyright © 2010 Pearson Education, Inc. 9-1 Linear Momentum Change in momentum: (a) mv (b) 2mv Copyright © 2010 Pearson Education, Inc. 9-2 Momentum and Newton’s Second Law Newton’s second law, as we wrote it before: is only valid for objects that have constant mass. Here is a more general form, also useful when the mass is changing: Copyright © 2010 Pearson Education, Inc. 9-3 Impulse Impulse is a vector, in the same direction as the average force. Copyright © 2010 Pearson Education, Inc. 9-3 Impulse We can rewrite as So we see that The impulse is equal to the change in momentum. Copyright © 2010 Pearson Education, Inc. 9-3 Impulse Therefore, the same change in momentum may be produced by a large force acting for a short time, or by a smaller force acting for a longer time. Copyright © 2010 Pearson Education, Inc. 9-4 Conservation of Linear Momentum The net force acting on an object is the rate of change of its momentum: If the net force is zero, the momentum does not change: Copyright © 2010 Pearson Education, Inc. 9-4 Conservation of Linear Momentum Internal Versus External Forces: Internal forces act between objects within the system. As with all forces, they occur in action-reaction pairs. As all pairs act between objects in the system, the internal forces always sum to zero: Therefore, the net force acting on a system is the sum of the external forces acting on it. Copyright © 2010 Pearson Education, Inc. 9-4 Conservation of Linear Momentum Furthermore, internal forces cannot change the momentum of a system. However, the momenta of components of the system may change. Copyright © 2010 Pearson Education, Inc. 9-4 Conservation of Linear Momentum An example of internal forces moving components of a system: Copyright © 2010 Pearson Education, Inc. 9-5 Inelastic Collisions Collision: two objects striking one another Time of collision is short enough that external forces may be ignored Inelastic collision: momentum is conserved but kinetic energy is not Completely inelastic collision: objects stick together afterwards Copyright © 2010 Pearson Education, Inc. 9-5 Inelastic Collisions A completely inelastic collision: Copyright © 2010 Pearson Education, Inc. 9-5 Inelastic Collisions Solving for the final momentum in terms of the initial momenta and masses: Copyright © 2010 Pearson Education, Inc. 9-5 Inelastic Collisions Ballistic pendulum: the height h can be found using conservation of mechanical energy after the object is embedded in the block. Copyright © 2010 Pearson Education, Inc. 9-5 Inelastic Collisions For collisions in two dimensions, conservation of momentum is applied separately along each axis: Copyright © 2010 Pearson Education, Inc. 9-6 Elastic Collisions In elastic collisions, both kinetic energy and momentum are conserved. One-dimensional elastic collision: Copyright © 2010 Pearson Education, Inc. 9-6 Elastic Collisions We have two equations (conservation of momentum and conservation of kinetic energy) and two unknowns (the final speeds). Solving for the final speeds: Copyright © 2010 Pearson Education, Inc. 9-6 Elastic Collisions Two-dimensional collisions can only be solved if some of the final information is known, such as the final velocity of one object: Copyright © 2010 Pearson Education, Inc. 9-7 Center of Mass The center of mass of a system is the point where the system can be balanced in a uniform gravitational field. Copyright © 2010 Pearson Education, Inc. 9-7 Center of Mass For two objects: The center of mass is closer to the more massive object. Copyright © 2010 Pearson Education, Inc. 9-7 Center of Mass The center of mass need not be within the object: Copyright © 2010 Pearson Education, Inc. 9-7 Center of Mass Motion of the center of mass: Copyright © 2010 Pearson Education, Inc. 9-7 Center of Mass The total mass multiplied by the acceleration of the center of mass is equal to the net external force: The center of mass accelerates just as though it were a point particle of mass M acted on by Copyright © 2010 Pearson Education, Inc. 9-8 Systems with Changing Mass: Rocket Propulsion If a mass of fuel Δm is ejected from a rocket with speed v, the change in momentum of the rocket is: The force, or thrust, is Copyright © 2010 Pearson Education, Inc. Summary of Chapter 9 • Linear momentum: • Momentum is a vector • Newton’s second law: • Impulse: • Impulse is a vector • The impulse is equal to the change in momentum • If the time is short, the force can be quite large Copyright © 2010 Pearson Education, Inc. Summary of Chapter 9 • Momentum is conserved if the net external force is zero • Internal forces within a system always sum to zero • In collision, assume external forces can be ignored • Inelastic collision: kinetic energy is not conserved • Completely inelastic collision: the objects stick together afterward Copyright © 2010 Pearson Education, Inc. Summary of Chapter 9 • A one-dimensional collision takes place along a line • In two dimensions, conservation of momentum is applied separately to each • Elastic collision: kinetic energy is conserved • Center of mass: Copyright © 2010 Pearson Education, Inc. Summary of Chapter 9 • Center of mass: Copyright © 2010 Pearson Education, Inc. Summary of Chapter 9 • Motion of center of mass: • Rocket propulsion: Copyright © 2010 Pearson Education, Inc.

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